US6655495B2 - Loudspeaker damper and loudspeaker - Google Patents

Abstract

A damper 3A is provided with an inner peripheral waveform portion 11 and an outer peripheral waveform portion 12. A flat portion 10 is provided between the inner peripheral waveform portion 11 and the outer peripheral waveform portion 12. When the damper is used for a loudspeaker, the flat portion 10 does not elastically deform in a radial direction R, so that linearity of the damper 3A in a vibrating direction Z is ensured by elastic deformation of the waveform portions. In addition, a rolling phenomenon of a voice coil bobbin and a diaphragm can be suppressed.

Description

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a loudspeaker damper serving as a supporting system of diaphragm and a loudspeaker using the damper.

2. Description of the Related Art

A structure of a conventional loudspeaker and a loudspeaker damper will be described. FIG. 1 is a cross-sectional view showing a structure of a loudspeaker using a conventional damper. As shown in FIG. 1, the loudspeaker includes avoice coil bobbin1, adiaphragm2, a damper3P, anedge4 and aframe5. A reference letter Z shown in FIG. 1 indicates a direction that thevoice coil bobbin1 vibrates during operation of the loudspeaker, and a reference letter R indicates a direction perpendicular to the Z direction, i.e., a radial direction of loudspeaker.

A voice coil1ais wound around a lower portion of thevoice coil bobbin1. Thevoice coil bobbin1 is elastically held, together with thediaphragm2, at theframe5 by the damper3P. An outer peripheral portion of thediaphragm2 is supported to theframe5 by theedge4 so as to vibrate. Amagnet6, ayoke7 and aplate8 constitute a magnetic circuit and a magnetic flux is generated at amagnetic gap9. When a signal current is applied to the voice coil1aplaced within themagnetic gap9, thevoice coil bobbin1 vibrates, by means of the magnetic flux of themagnetic gap9, in the Z direction with a driving force which is proportional to the signal current. The vibration is transmitted to thediaphragm2, so that sound is radiated.

In accordance with such a conventional loudspeaker, in order to vibrate thevoice coil bobbin1 and thediaphragm2 so as to follow a signal current, a cross-sectional shape of the damper3P is formed in a wavy shape. Further, a radial direction of the damper is expandable and contractible. In this way, the damper3P easily vibrates in the Z direction.

In the case where the damper3P has a wavy cross-sectional shape, the damper3P easily vibrates also in the R direction. Ideally, thevoice coil bobbin1 and thediaphragm2 vibrate only in the Z direction in proportion to a signal current. In accordance with an actual loudspeaker, however, vibration in the R direction as well as the Z direction is induced due to variations in assembling of the loudspeaker and weight balance, and force applied to the loudspeaker depending on an installation method.

Vibration in the R direction is referred to as a rolling phenomenon. If the rolling phenomenon occurs, the voice coil1aabuts theyoke7 or theplate8 at a time of operation of the loudspeaker, so that unpleasant noise is generated or the voice coil1ais broken. If themagnetic gap9 is broaden in order to prevent such abutment of the voice coil1a, an efficiency of electro acoustic conversion of the loudspeaker is reduced. Accordingly, if the rolling phenomenon can be suppressed while maintaining a distance of themagnetic gap9 at a predetermined value, generation of unpleasant noise and failure of the voice coil1acan be prevented and a high performance loudspeaker with high efficiency can be realized.

SUMMARY OF THE INVENTION

A loudspeaker damper of the present invention is configured by an annular member so as to have a central opening portion, and is provided with an outer peripheral waveform portion which has at least one concave or convex annular waveform at an outer peripheral portion, an inner peripheral waveform portion which has at least one concave or convex annular waveform at an inner peripheral portion, and a flat portion which is provided between the outer peripheral waveform portion and the inner peripheral waveform portion and has an annular flat surface.

A loudspeaker of the present invention is provided with a loudspeaker frame, a diaphragm which has an outer peripheral portion held by the loudspeaker frame so as to vibrate and applies aerial vibration, a cylindrical voice coil bobbin which is coupled to an inner peripheral portion of the diaphragm, a voice coil which is wound around the voice coil bobbin, a magnetic circuit which applies an electromagnetic force to the voice coil and a damper which has an outer peripheral portion held by the loudspeaker frame so as to vibrate and holds the voice coil bobbin so as to axially vibrate.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross-sectional view showing a structure of a conventional loudspeaker using a waveform damper;

FIG. 2 is a cross-sectional view showing a structure of a virtual loudspeaker using a flat damper;

FIG. 3 is a characteristic view showing the relationship between a radial position and a stress distribution when the flat damper is vibrated;

FIG. 4 is a plan view showing a structure of a loudspeaker damper according toEmbodiment 1 of the present invention;

FIG. 5 is a cross-sectional view showing the structure of the loudspeaker damper according toEmbodiment 1;

FIG. 6 is a characteristic view showing the relationship between an amplitude characteristic of a diaphragm of a loudspeaker, and a minimum resonance frequency and a rolling frequency;

FIG. 7 is an explanatory view showing a shape and a dimension of a conventional damper;

FIG. 8 is an explanatory view showing a shape and a dimension of the damper according toEmbodiment 1;

FIG. 9 is a characteristic view showing the relationship between a driving force for the diaphragm and a displacement amount in the conventional loudspeaker and the loudspeaker according toEmbodiment 1;

FIG. 10 is a plan view showing a structure of a loudspeaker damper according toEmbodiment 2 of the present invention;

FIG. 11 is a cross-sectional view taken along line O-P, showing the structure of the loudspeaker damper according toEmbodiment 2;

FIG. 12 is a cross-sectional view taken along line O-Q, showing the structure of the loudspeaker damper according toEmbodiment 2;

FIG. 13 is a plan view showing a structure of a loudspeaker damper with another shape according toEmbodiment 2 of the present invention;

FIG. 14 is a cross-sectional view taken along line O-P, showing the structure of the loudspeaker damper with another shape according toEmbodiment 2;

FIG. 15 is a cross-sectional view taken along line O-Q, showing the structure of the loudspeaker damper with another shape according toEmbodiment 2;

FIG. 16 is a cross-sectional view showing a structure of a loudspeaker damper according toEmbodiment 3 of the present invention;

FIG. 17 is a plan view showing a structure of a loudspeaker damper according toEmbodiment 4 of the present invention;

FIG. 18 is a cross-sectional view showing the structure of the loudspeaker damper according toEmbodiment 4;

FIG. 19 is a cross-sectional view showing a structure of a loudspeaker damper with another shape (1) according toEmbodiment 4;

FIG. 20 is a cross-sectional view showing a structure of a loudspeaker damper with still another shape (2) according toEmbodiment 4;

FIG. 21 is a plan view showing a structure of a loudspeaker damper with yet another shape (3) according toEmbodiment 4;

FIG. 22 is a cross-sectional view taken along line O-P, showing the structure of the loudspeaker damper with yet another shape (3) according toEmbodiment 4;

FIG. 23 is a cross-sectional view showing a structure of a loudspeaker damper with yet another shape (4) according toEmbodiment 4;

FIG. 24 is a plan view showing a structure of a loudspeaker damper according toEmbodiment 5 of the present invention;

FIG. 25 is a cross-sectional view taken along line O-P, showing the structure of the loudspeaker damper according toEmbodiment 5;

FIG. 26 is a cross-sectional view taken along line A-B, showing the structure of the loudspeaker damper according toEmbodiment 5;

FIG. 27 is a cross-sectional view taken along line A-B, showing a structure of a loudspeaker damper with another shape (1) according toEmbodiment 5;

FIG. 28 is a cross-sectional view taken along line A-B showing a structure of a loudspeaker damper with still another shape (2) according toEmbodiment 5;

FIG. 29 is a cross-sectional view taken along line A-B showing a structure of a loudspeaker damper with yet another shape (3) according toEmbodiment 5;

FIG. 30 is a plan view showing a structure of a loudspeaker damper with yet another shape (4) according toEmbodiment 5;

FIG. 31 is a perspective view showing a protruding portion of the loudspeaker damper with yet another shape (4) according toEmbodiment 5;

FIG. 32 is a cross-sectional view taken along line O-P, showing the structure of the loudspeaker damper with yet another shape (4) according toEmbodiment 5;

FIG. 33 is a cross-sectional view taken along line A-B, showing the structure of the loudspeaker damper with yet another shape (4) according toEmbodiment 5;

FIG. 34 is a partial cross-sectional view of radial protruding portions showing a structure of a loudspeaker damper with yet another shape (5) according toEmbodiment 5;

FIG. 35 is a cross-sectional view showing a structure of a loudspeaker according to Embodiment 6-1 of the present invention; and

FIG. 36 is a cross-sectional view showing a structure of a loudspeaker according to Embodiment 6-2 of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

FIG. 2 is a cross-sectional view of a virtual loudspeaker using a flat plate damper. If a damper3Q is configured as completely flat surface as in a case of the loudspeaker shown in FIG. 2, the damper3Q is difficult to move in an R direction, so that the rolling phenomenon can be suppressed. At the same time, however, the damper3Q is difficult to move in a Z direction. Thus, linearity of amplitude of adiaphragm2 with respect to driving force cannot be obtained. Further, tone quality of the loudspeaker is significantly deteriorated and maximum sound pressure is also reduced.

FIG. 3 is a characteristic view showing the relationship between a radial position of the damper and a stress applied to a portion of the damper placed at the radial position. The relationship is obtained as follows. Firstly, the flat damper3Q used in the loudspeaker of FIG. 2 is determined as an object of analysis. Then, an outer periphery of the damper is fixed and a Z direction force is applied to an inner periphery of the damper such that each of the portions of the damper is displaced in the Z direction. A horizontal axis shown in FIG. 3 indicates a radial position of the respective portions of the damper, and a vertical axis indicates a stress applied to the respective portions of the damper. As shown in the characteristic view, the portions with large stress are an outer peripheral portion and an inner peripheral portion of the damper. Accordingly, such portions are formed in a wavy shape so as to easily move in the Z direction and other portions are formed in a planar shape not so as to move in the R direction. As a result, the rolling phenomenon can be suppressed and an excellent damper that a linearity of amplitude of diaphragm is not deteriorated can be realized.

A loudspeaker and a loudspeaker damper according to embodiments of the present invention will be described with reference to the drawings. The same elements as those of a conventional loudspeaker shown in FIG. 1 are denoted by the same reference numerals, so that detailed description thereof will not be repeated.

(Embodiment 1)

FIG. 4 is a plan view showing a structure of a loudspeaker damper according toEmbodiment 1 of the present invention. In the following description, a loudspeaker damper will be simply referred to as a damper. FIG. 5 is a cross-sectional view showing a shape of damper, cut so as to include a central axis of the damper. A damper3A of this embodiment is, as shown in FIG. 4, configured by an annular member so as to have a hollow opening portion. A waveform portion is formed at an inner peripheral portion of the damper and this waveform portion is referred to as an innerperipheral waveform portion11. A waveform portion is also formed at an outer peripheral portion thereof and this waveform portion is referred to as an outerperipheral waveform portion12. Such concave or convex annular grooves are referred to as annular waveforms.

Aflat portion10 which has an annular flat surface parallel to a radial direction of the damper is formed between the innerperipheral waveform portion11 and the outerperipheral waveform portion12. An inner side of the innerperipheral waveform portion11 is open so as to become a complete round such that thevoice coil bobbin1 can be fixed thereto. In a case of assembling the damper3A into a loudspeaker, as shown in FIG. 5, a direction that thevoice coil bobbin1 vibrates is determined as the Z direction and a radial direction of the damper3A is determined as the R direction.

Effects of the damper with such structure will be described. Because theflat portion10 is provided, the damper3A hardly expands or contracts in the R direction. With respect to the direction that thevoice coil bobbin1 vibrates, due to the inner and outerperipheral waveform portions11 and12, the inner and outer peripheral portions receiving a large stress can easily move. For this reason, elastic fatigue of material of the damper can be reduced and vibration of the damper3A in the Z direction is hardly prevented. As a result, thevoice coil bobbin1 hardly induces the rolling phenomenon, so that the loudspeaker damper with excellent linearity can be obtained.

FIG. 6 is a frequency characteristic view showing a vibration amplitude of voice coil of a loudspeaker when a certain signal current is applied thereto. At a horizontal axis, a frequency is indicated by logarithm (log frequency). A vertical axis indicates a relative amplitude value. A reference letter C in FIG. 6 indicates an amplitude value. A reference letter D indicates a minimum resonance frequency of the loudspeaker, a reference letter E indicates a frequency at which rolling of the conventional waveform damper occurs most (which hereinafter is referred to as rolling frequency) and a reference letter F indicates a rolling frequency when the damper according toEmbodiment 1 is used.

In general, an amplitude of the diaphragm of the loudspeaker attenuates at a rate of 12 dB per octave at the area with minimum resonance frequency or higher. For this reason, higher the frequency is, smaller the amplitude is. Thus, by increasing a rolling frequency, an amount of amplitude of rolling can be minimized. Consequently, a magnetic gap needs not to be made narrow more than needed and contact of voice coil can be prevented. For example, a case of applying conventional damper to a loudspeaker is compared to a case of applying a damper ofEmbodiment 1 to a loudspeaker. The conventional damper and the damper ofEmbodiment 1 have the same total length seen from a cross section thereof (i.e., the same outer diameter dimension).

The following table shows a ratio Ra of rolling frequency to minimum resonance frequency, a rolling frequency f_Rwith the minimum resonance frequency being 100 Hz, an R direction amplitude amount A_Rin the rolling frequency and a Z direction maximum amplitude amount A_z.

	TABLE 1
	Ra	fR	AR	Az

	Conventional	4.82	482 Hz	100%	100%
	Example
	Embodiment
1	5.79	579 Hz	75.8%	100%

FIG. 7 shows dimensions of a part of a voice coil bobbin and main portions of the conventional damper3P. FIG. 8 shows dimensions of a part of the voice coil bobbin and the main portions of damper3A ofEmbodiment 1. A unit is mm. FIG. 9 shows the relationship between a driving force and a Z direction displacement amount of the inner peripheral portions of the dampers3P and3A when a Z direction driving force is applied to thevoice coil bobbin1. Referring to FIG.9 and the above table, the damper3A ofEmbodiment 1 can obtains excellent effects in that the rolling phenomenon is suppressed without reducing a maximum amplitude of diaphragm.

The damper3P shown in FIG. 1 has totally ten convexes and concaves. In contrast, the damper3A shown in FIG. 4 has three concaves and convexes at the innerperipheral waveform portion11 and three concaves and convexes at the outerperipheral waveform portion12, i.e., has totally six annular waveforms. Theflat portion10 is formed such that an outer diameter of the damper is not changed and the number of convexes and concaves is reduced. The number of annular waveforms may be any number and can be appropriately selected depending on easiness of manufacturing, linearity with respect to amplitude and shape of loudspeaker. In accordance with results of various trials, it has been found that an annular width W of theflat portion10 is preferably equal to or larger than a groove width of annular waveform of the outer peripheral waveform portion or the inner peripheral waveform portion.

Theflat portion10 may be made of materials having higher Young's modulus than materials for the inner and outer peripheral waveform portions. For example, theflat portion10 is made of plastic and the innerperipheral waveform portion11 and the outerperipheral waveform portion12 are made of fabrics. Young's modulus on radial direction of the flat portion may be larger than at least one of Young's modulus on radial direction of the outer peripheral waveform portion and a Young's modulus on radial direction of said inner peripheral waveform portion. Thus, stiffness of theflat portion10 becomes larger and the effect of suppressing the rolling phenomenon can be even further enhanced.

(Embodiment 2)

Next, a damper according toEmbodiment 2 of the present invention will be described. FIG. 10 is a plan view showing a structure of damper ofEmbodiment 2. FIG. 11 is a cross-sectional view taken along line O-P shown in FIG.10. FIG. 12 is a cross-sectional view taken along line O-Q shown in FIG.10. The damper3B is configured by an annular member with elliptic outline. As inEmbodiment 1, complete round shaped opening is formed at an inner peripheral portion of the damper3B such that thevoice coil bobbin1 is attached thereto. The damper3B includes a flat portion10A with elliptic outer peripheral profile, an outer peripheral waveform portion12A with elliptic outer peripheral and inner peripheral profiles and an inner peripheral waveform portion11A whose outer peripheral profile fits the flat portion10A. As shown in FIG. 10, a direction of short axis of the damper is indicated by S and a direction of long axis of the damper is indicated by L. As seen from comparison between FIG.11 and FIG. 12, a width of concave or convex of each waveform portion and a distance between concaves or convexes vary significantly particularly in the L axis direction.

Effects of the damper with such structure will be described. Stiffness of elliptic damper is governed by a shape in the short axis direction. By setting an area of the flat portion10A in the long axis direction to be large, as compared to an elliptic damper with ordinary waveform, the rolling phenomenon can be suppressed without varying significantly the minimum resonance frequency of the loudspeaker.

FIGS. 13,14 and15 show another structural examples of the damper ofEmbodiment 2. FIG. 13 is a plan view of damper3C. FIG. 14 is a cross-sectional view taken along line O-P shown in FIG.13. FIG. 15 is a cross-sectional view taken along line O-Q shown in FIG.13. As shown in FIG. 13, the damper3C includes a flat portion10B, an inner peripheral waveform portion11B and an outer peripheral waveform portion12B. As shown in FIG. 13, a short diameter of outer periphery of the flat portion10B may be the same as a short diameter of inner periphery thereof. Also with such structure, the rolling phenomenon can be suppressed without varying significantly the minimum resonance frequency of the loudspeaker.

(Embodiment 3)

Next, a damper according toEmbodiment 3 of the present invention will be described. FIG. 16 is a cross-sectional view showing a structure of damper according toEmbodiment 3. The damper3D includes a flat portion10C, an inner peripheral waveform portion11C and an outer peripheral waveform portion12C. An inner connecting portion13 is formed at a boundary portion between the flat portion10C and the inner peripheral waveform portion11C. An outer connecting portion14 is formed at a boundary portion between the flat portion10C and the outer peripheral waveform portion12C. A reference letter Z shown in FIG. 16 indicates a direction that a voice coil vibrates in a case of using the damper3D for a loudspeaker. A reference letter R indicates a radial direction of the damper3D.

The inner connecting portion13 is configured by an annular waveform having a height (depth) equal to or lower than a groove height (or a groove depth) of a concave or a convex of the inner and outer peripheral waveform portions. The inner connecting portion13 connects the inner peripheral waveform portion11C to an inner periphery of the flat portion10C. The outer connecting portion14 is configured by an annular waveform having a groove height equal to or lower than an amplitude of a concave or a convex of the inner and outer peripheral waveform portions. The outer connecting portion14 connects the outer peripheral waveform portion12C to an outer periphery of the flat portion10C.

By providing the flat portion10C as in the above-described embodiments, the damper3D hardly expands and contracts in the R direction. With respect to the direction Z that thevoice coil bobbin1 vibrates, a desired amplitude can be ensured by providing the inner peripheral waveform portion11C and the outer peripheral waveform portion12C. When portions of flat damper with large stress shown in FIG. 3 are made to be easily movable, elastic fatigue of damper material can be reduced. For this reason, limitation of amplitude of vibration at the inner peripheral portion of the damper3D is relaxed. As a result, the rolling phenomenon hardly occurs and a loudspeaker damper with excellent linearity can be obtained. Such effects are the same as inEmbodiment 1.

Further, the flat portion10C is connected via the inner connecting portion13 to the inner peripheral waveform portion11C. The flat portion10C is also connected via the outer connecting portion14 to the outer peripheral waveform portion12C. Accordingly, the inner peripheral waveform portion11C and the outer peripheral waveform portion12C are easy to move and a linearity is improved. When a large input is applied and vibration occurs with large amplitude, as compared to the case in which the inner and outer connecting portions are not provided, a stress applied to connecting portions of the flat portion and the waveform portion can be distributed. Consequently, durability of damper is improved, and elastic fatigue of connecting portions and break thereof can be prevented.

Referring to FIG. 16, although the number of convexes and concaves of the inner connecting portion13 and the outer connecting portion14 is two, any number of concaves and convexes may be used. If Young's modulus on radial direction of the outer connecting portion and the inner connecting portion are smaller than Young's modulus on radial direction of the outer peripheral waveform portion and the inner peripheral waveform portion, mobility and linearity are even further improved. If viscoelasticities of the outer connecting portion and the inner connecting portion are larger than radial viscoelasticities of the outer peripheral waveform portion and the inner peripheral waveform portion, distortion due to stress can be absorbed by internal loss. At this time, durability of damper is even further improved. Further, linearity, rolling suppressing effect, durability and easiness of manufacturing of damper are improved depending on materials and shapes selected, and a minimum resonance frequency of loudspeaker can be finely adjusted.

(Embodiment 4)

Next, a damper according toEmbodiment 4 of the present invention will be described. FIG. 17 is a plan view showing a structure of damper ofEmbodiment 4. FIG. 18 is a cross-sectional view taken along line O-P shown in FIG.17. The damper3E includes aflat portion10D, an inner peripheral waveform portion11D and an outer peripheral waveform portion12D. A large number of protrudingportions15 are provided at theflat portion10D. In accordance withEmbodiment 4, the protrudingportions15 are formed in a hemispherical shape. Diameters of the protrudingportions15 and their positions are random. A reference letter Z shown in FIG. 18 indicates a direction that a voice coil vibrates when the damper3E is assembled into a loudspeaker. A reference letter R indicates a radial direction of the damper.

Effects of the damper with such structure will be described. By providing theflat portion10D, the damper3E hardly expands and contracts in the R direction. With respect to a direction that a voice coil bobbin vibrates, a desired amplitude is ensured by providing the inner peripheral waveform portion11D and the outer peripheral waveform portion12D. Further, portions of flat damper with large stress shown in FIG. 3 are made to be easily movable, so that elastic fatigue of damper material can be reduced. Thus, vibration of the damper3E is not suppressed. Further, the rolling phenomenon hardly occurs and a loudspeaker damper with excellent linearity can be obtained. In this way, the same effects as those ofEmbodiment 1 can be obtained.

Theflat portion10D easily resonates, because of its cross-sectional shape, at a frequency that a peripheral width W is ½ wavelength. For this reason, a tone quality of loudspeaker may be deteriorated by resonance. A resonance point can be distributed by providing protruding portions shown in FIGS. 17 and 18 at theflat portion10D. As a result, deterioration of tone quality at a specific resonance frequency can be prevented. Because a strength in the R direction is increased due to the protruding portions, the rolling phenomenon can be suppressed. Referring to FIGS. 17 and 18, the protrudingportions15 are provided so as to protrude upward. Nevertheless, the same effect can be obtained if the protruding portions are provided so as to protrude downward.

FIGS. 19 through 23 are views showing another structural examples of the damper ofEmbodiment 4. FIG. 19 is a cross-sectional view showing a structure of damper3F having hollow protruding portions. The damper3F shown in FIG. 19 includes a flat portion10E, an inner peripheral waveform portion11E and an outer peripheral waveform portion12E. A plurality of hemispherical shell protruding portions15A may be provided at one surface of the flat portion10E or may be provided at opposite surfaces thereof.

FIG. 20 is a cross-sectional view showing a structure of damper3G having a plurality of filled protruding portions (which hereinafter refers to as solid protruding portions). The damper3G shown in FIG. 20 includes a flat portion10F, an inner peripheral waveform portion11F and an outer peripheral waveform portion12F. A plurality of hemispherical filled protruding portions15B are provided at the flat portion10F. When a damper is formed by pressing a sheet material with uniform thickness into a die, an interior of each of protruding portions is a cavity as shown in FIG.19. When a damper is die-formed by injecting a resin, an interior of each of the protruding portions is filled with resin as shown in FIG. 20. A designer can freely select materials by taking weight of damper, resonance suppressing effect, rolling suppressing effect and formability into consideration.

FIG. 21 is a plan view showing a structure of damper3H having a plurality of stripe-shaped protruding portions with triangular cross-sectional shape. FIG. 22 is a cross-sectional view taken along line O-P shown in FIG.21. The damper3H shown in FIGS. 21 and 22 includes aflat portion10G, an inner peripheral waveform portion11G and an outer peripheral waveform portion12G. A plurality of stripe-shaped protruding portions15C with triangular cross-sectional shape are provided at theflat portion10G. A length, a direction and a position of each of the protruding portions15C are at random as shown in FIG.21.

FIG. 23 is a cross-sectional view showing a structure of damper3I having a plurality of stripe-shaped protruding portions with rectangular cross-sectional shape. The damper3I shown in FIG. 23 includes aflat portion10H, an inner peripheral waveform portion11H and an outerperipheral waveform portion12H. A plurality of stripe-shaped protruding portions with rectangular cross-sectional shape are provided at theflat portion10H. The stripe-shaped protrudingportions15 are placed at random. These stripe-shaped protruding portions may be made of materials different from the damper3H or3I and may be affixed to the annular flat surface. For example, portions other than the stripe-shaped protruding portions are integrally formed of fabrics and the stripe-shaped protruding portions are formed of plastic or aluminum. Then, the stripe-shaped protruding portions may be affixed to theflat portion10H. If the stripe-shaped protruding portion is made of materials with high Young's modulus, an effect of reinforcing the flat portion is enhanced. Further, effects of suppressing the rolling phenomenon and resonance can be obtained. Alternatively, if the stripe-shaped protruding portion is made of material with high viscoelasticity, e.g., a rubber, the Q factor of resonance of the flat portion can be reduced and an effect of suppressing resonance can be obtained. The stripe-shaped protruding portions may have hemispherical cross-sectional shape or any polygonal cross-sectional shape.

(Embodiment 5)

A damper ofEmbodiment 5 of the present invention will be described. FIG. 24 is a plan view showing a structure of damper ofEmbodiment 5. FIG. 25 is a cross-sectional view taken along line O-P shown in FIG.24. FIG. 26 is a cross-sectional view taken along line A-B shown in FIG.24. The damper3J includes a flat portion10J, an inner peripheral waveform portion11J and an outer peripheral waveform portion12J. A plurality of radial protrudingportions16 are provided at the flat portion10J. Each of the radial protrudingportions16 has, as shown in FIG. 26, a triangular cross-sectional shape and is formed in a hollow stripe shape. As shown in FIG. 24, theradial protruding portions16 are radially disposed along a radial direction of the damper3J. A reference letter Z shown in FIG. 25 indicates a direction that a voice coil vibrates when the damper3J is assembled into a loudspeaker. A reference letter R indicates a radial direction of the damper3J.

Effects of the damper with above-described structure will be described. Because the flat portion10J is provided, the damper3J hardly expands or contracts in the R direction. With respect to the direction Z that a voice coil bobbin vibrates, because of the inner peripheral waveform portion11J and the outer peripheral waveform portion12J, portions of flat damper that receive a large stress easily move. For this reason, an amplitude of the damper3J at a time of its vibration is ensured. The rolling phenomenon hardly occurs and a loudspeaker damper with excellent linearity can be obtained. In this way, the same effects as inEmbodiment 1 can be obtained.

The flat portion easily resonates, due to its cross-sectional shape, at a frequency that a peripheral width W serves as ½ wavelength. A tone quality of loudspeaker may be deteriorated by such resonance. As the flat portion10J ofEmbodiment 5 is provided with the radial protrudingportions16, the flat portion10J is reinforced and thus resonance can be suppressed. A strength in the R direction is increased because of the radial protrudingportions16, an effect of suppressing the rolling phenomenon is enhanced. This effect is the same as that ofEmbodiment 3.

FIGS. 27 through 29 show another structural examples of the radial protruding portion. Referring to FIG. 26, the hollowradial protruding portions16 are provided so as to protrude upward from the flat portion10J. Nevertheless, as in a flat portion10K shown in FIG. 27, the same effect can be obtained when radial protruding portions16A are protruded upward and downward. Alternatively, the radial protruding portions may be protruded upward and downward and alternately disposed along a circumferential direction.

As shown by a flat portion10L of FIG. 28, each of radial protruding portions16B may have a hollow rectangular cross-sectional shape. Further, as shown by aflat portion10M of FIG. 29, each of radial protruding portions16C may have a solid triangular cross-sectional shape. A designer can freely select these shapes by taking easiness of forming, effect of suppressing resonance of flat portion, effect of suppressing the rolling phenomenon and weight of damper into consideration.

The radial protruding portions ofEmbodiment 5 may be formed of other materials and affixed to the flat portion. For example, portions other than the radial protruding portions are integrally formed of fabrics and the radial protruding portions are formed of plastic or aluminum. Then, the radial protruding portions may be applied to the flat portion. If the radial protruding portion is made of materials with high Young's modulus as described above, the effect of reinforcing the flat portion is enhanced and effects of suppressing the rolling phenomenon and resonance can be obtained. If the radial protruding portion is made of material with high viscoelasticity, e.g., a rubber, sharpness of resonance of the flat portion can be reduced and the effect of suppressing the resonance is enhanced.

FIGS. 30 through 33 show another structural examples of the damper ofEmbodiment 5. FIG. 30 is a plan view showing a structure of damper3L. FIG. 31 is a perspective view of protruding portion. FIG. 32 is a cross-sectional view taken along line O-P shown in FIG.30. FIG. 33 is a cross-sectional view taken along line A-B, i.e., a cross-sectional view showing a center of protruding portion along a circumferential direction. The damper3L includes a flat portion10N, an inner peripheral waveform portion11K and an outer peripheral waveform portion12K. A plurality of quadrangular pyramid shaped protruding portions16D are provided at the flat portion10N.

As shown in FIGS. 30 and 31, each of the protruding portions16D has a rhombic bottom surface and a hollow quadrangular pyramid shape. Because the protruding portions16D with such shape even further reinforce the flat portion, effects of suppressing the resonance of the flat portion10N and the rolling phenomenon can be obtained. Although the protruding portions16D are provided so as to protrude upward in FIG. 33, the protruding portions16D may be provided so as to protrude downward.

FIG. 34 shows a cross-sectional view of the same portion showing another structural example of the protruding portion. The protruding portions16E are formed so as to alternately protrude upward and downward from the flat portion10P. In this case, the same effect can be obtained.

(Embodiment 6)

Next, a loudspeaker to which the damper of the above-described embodiments is mounted will be described asEmbodiment 6 of the present invention. FIG. 35 is a cross-sectional view showing a structure of loudspeaker of Embodiment 6-1. The same portions as those of loudspeaker shown in FIG. 1 are indicated by the same reference numerals. The loudspeaker is configured so as to include avoice coil bobbin1, adiaphragm2, a damper3A, anedge4 and aframe5.

Thevoice coil bobbin1 is held by a coaxial damper3A ofEmbodiment 1. Thevoice coil bobbin1 is supported, together with thediaphragm2, by theframe5 so as to freely vibrate. An outer peripheral portion of thediaphragm2 is supported to theframe5 by the roll-shapededge4.

A magnetic circuit is formed by amagnet6, ayoke7 and aplate8. A desired magnetic flux density is ensured at amagnetic gap9 of the magnetic circuit. The voice coil1ais held within themagnetic gap9. A reference letter Z shown in FIG. 35 indicates a direction that the voice coil bobbin vibrates and a reference letter R indicates a radial direction of the damper, which is perpendicular to the vibrating direction.

An operation of the loudspeaker with such structure will be described. When a signal current is applied to the voice coil1a, thevoice coil bobbin1 vibrates, due to a magnetic flux of themagnetic gap9, at a driving force which is in proportion to the signal current. This vibration is transmitted to thediaphragm2, so that sound is radiated.

As shown in FIG. 35, when the damper ofEmbodiment 1 is used, the rolling phenomenon of loudspeaker can be effectively suppressed. The same effects can be obtained when dampers ofEmbodiments 2 through 5 are used.

FIG. 36 is a cross-sectional view of loudspeaker of Embodiment 6-2, and the same portions as in FIG. 35 are indicated by the same reference numerals. As shown in FIG. 36, a first damper3M and a second damper3N may be used instead of one damper. In accordance with a loudspeaker shown in FIG. 36, since thevoice coil bobbin1 is supported by the first damper3M and the second damper3N, an effect of suppressing the rolling phenomenon is significantly enhanced. When an upper limit value of elastic deformation of one damper is limited to a predetermined value, over amplitude of the diaphragm at an over input can be suppressed and deterioration of performance of loudspeaker can be prevented.

Two dampers may be provided by combining the same damper shown in one ofEmbodiments 1 through 5 or any of two dampers ofEmbodiments 1 through 5. A designer can freely select dampers by taking the effect of suppressing the rolling phenomenon and linearity in the vibrating direction into consideration.

As described above, in accordance with a loudspeaker damper, a flat portion is provided between an outer peripheral waveform portion and an inner peripheral waveform portion. Thus, the rolling phenomenon of diaphragm and voice coil bobbin can be suppressed. Further, linearity of vibration of diaphragm from a small amplitude to a large amplitude can be realized.

Since protruding portions are provided at a flat portion of damper, a stiffness of the flat portion is improved and resonance of the flat portion can be suppressed. At this time, deterioration of tone quality caused by resonance of the flat portion can be prevented.

In accordance with a loudspeaker of the present invention, the rolling phenomenon can be suppressed even if a diaphragm vibrates at a large amplitude. Accordingly, contact of voice coil when driven at large electric power is eliminated. Further, a positional precision at a time of mounting a voice coil bobbin and a damper to a magnetic circuit is relaxed, and a manufacturing yield of loudspeaker is improved.

It is to be understood that although the present invention has been described with regard to preferred embodiments thereof, various other embodiments and variants may occur to those skilled in the art, which are within the scope and spirit of the invention, and such other embodiments and variants are intended to be covered by the following claims.

The text of Japanese priority application No. 2001-317960 filed on Oct. 16, 2001 is hereby incorporated by reference.

Claims (18)

What is claimed is:

1. A loudspeaker damper for use in a loudspeaker having a diaphragm and a voice coil bobbin, said damper including:

an annular member so as to have a central opening portion for connecting to the voice coil bobbin, said annular member comprising:

an outer peripheral waveform portion which has at least one concave or convex annular waveform at an outer peripheral portion;

an inner peripheral waveform portion which has at least one concave or convex annular waveform at an inner peripheral portion around said central opening portion; and

a flat portion which is provided between said outer peripheral waveform portion and said inner peripheral waveform portion and has an annular flat surface.

2. A loudspeaker damper according toclaim 1, wherein

an annular width of said flat portion is equal to or more than a groove width of the annular waveform of said outer peripheral waveform portion or said inner peripheral waveform portion.

3. A loudspeaker damper according toclaim 1, wherein

inner and outer peripheral profiles of said outer peripheral waveform portion are formed in an elliptic shape and at least an outer peripheral profile of said flat portion is formed in an elliptic shape.

4. A loudspeaker damper according toclaim 1, wherein

a Young's modulus in a radial direction of said flat portion is larger than at least one of Young's modulus in a radial direction of said outer peripheral waveform portion and a Young's modulus in a radial direction of said inner peripheral waveform portion.

5. A loudspeaker damper according toclaim 1, wherein

an outer connecting portion with at least one concave or convex annular waveform is provided at an annular boundary between said flat portion and said outer peripheral waveform portion, and

an inner connecting portion with at least one concave or convex annular waveform is provided at an annular boundary between said flat portion and said inner peripheral waveform portion.

6. A loudspeaker damper according toclaim 5, wherein

a groove height of said concave or convex annular waveform of said outer connecting portion is lower than a groove height of the annular waveform of said outer peripheral waveform portion, and

a groove height of the annular waveform of said inner connecting portion is smaller than a groove height of the annular waveform of said inner peripheral waveform portion.

7. A loudspeaker damper according toclaim 5, wherein

a Young's modulus in a radial direction of said outer connecting portion and said inner connecting portion are smaller than a Young's modulus in a radial direction of said outer peripheral waveform portion and said inner peripheral waveform portion.

8. A loudspeaker damper according toclaim 5, wherein

viscoelasticities of said outer connecting portion and said inner connecting portion are larger than radial viscoelasticities of said outer peripheral waveform portion and said inner peripheral waveform portion.

9. A loudspeaker damper according toclaim 1, wherein

a plurality of protruding portions are provided on at least one of upper surface and lower surface of said flat portion for suppressing resonance of said flat portion.

10. A loudspeaker damper according toclaim 9, wherein

said protruding portions are radially disposed along an annular flat surface of said flat portion.

11. A loudspeaker damper according toclaim 9, wherein

said protruding portions are stripe-shaped protruding portions and have a polygonal cross-sectional shape.

12. A loudspeaker damper according toclaim 9, wherein

said protruding portions are stripe-shaped protruding portions radially formed on said annular flat surface of said flat portion and have a polygonal cross-sectional shape.

13. A loudspeaker damper according toclaim 12, wherein

said protruding portions are alternately disposed at the upper and lower surfaces of said flat portion so as to be adjacent to each other along a circumferential direction.

14. A loudspeaker damper according toclaim 9, wherein

said protruding portions are stripe-shaped protruding portions with random direction and length which are formed on said annular flat surface of said flat portion, and have a polygonal cross-sectional shape.

15. A loudspeaker damper according toclaim 9, wherein

said protruding portions are quadrangular pyramids having rhombic bottom surfaces disposed on the annular flat surface of said flat portion, and

said quadrangular pyramids are radially disposed along said annular flat surface.

16. A loudspeaker damper according toclaim 9, wherein

said protruding portions are made of any of materials including a metal, a polymer resin and an viscoelastic body.

17. A loudspeaker comprising:

a loudspeaker frame;

a diaphragm which has an outer peripheral portion held by said loudspeaker frame with an edge so as to vibrate and applies aerial vibration;

a cylindrical voice coil bobbin which is coupled to an inner peripheral portion of said diaphragm;

a voice coil which is wound around said voice coil bobbin;

a magnetic circuit which applies an electromagnetic force to said voice coil; and

a damper which has an outer peripheral portion held by said loudspeaker frame so as to vibrate and which has a central opening portion to hold said voice coil bobbin in the central opening so as to axially vibrate, wherein

said damper includes:

an outer peripheral waveform portion which has at least one concave or convex annular waveform at an outer peripheral portion;

an inner peripheral waveform portion which has at least one concave or convex annular waveform at an inner peripheral portion around the central opening portion; and

a flat portion which is provided between said outer peripheral waveform portion and said inner peripheral waveform portion and has an annular flat surface.

18. A loudspeaker comprising:

a loudspeaker frame;

a diaphragm which has an outer peripheral portion is held by said loudspeaker frame with an edge so as to vibrate and applies aerial vibration;

a cylindrical voice coil bobbin which is coupled to an inner peripheral portion of said diaphragm;

a voice coil which is wound around said voice coil bobbin;

a magnetic circuit which applies an electromagnetic force to said voice coil; and

first and second dampers which have outer peripheral portions held by said loudspeaker frame so as to freely vibrate, have inner peripheral portions fixed to two different axial positions of said voice coil bobbin, and have a central opening portion, respectively to hold said voice coil bobbin in the central opening so as to axially vibrate, wherein

said first and second dampers include:

an outer peripheral waveform portion which has at least one concave or concave annular waveform at an outer peripheral portion;

an inner peripheral waveform portion which has at least one concave or convex annular waveform at an inner peripheral portion around the central opening portion; and

a flat portion which is provided between said outer peripheral waveform portion and said inner peripheral waveform portion and has an annular flat surface.

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